This behavior can be modeled by solving the Burgers equation with random forcing, but more commonly modeled with the standard k-epsilon model.  The two-dimensional type of this phenomenon features an upscale energy cascade, a reversal of a concept originally proposed by Richardson.  Intermittency in this phenomenon is manifested in anomalous scaling of the velocity structure functions of order p. 
This behavior can be modeled by solving the Burgers equation with random forcing, but more commonly modeled with the standard k-epsilon model.  The two-dimensional type of this phenomenon features an upscale energy cascade, a reversal of a concept originally proposed by Richardson.  Intermittency in this phenomenon is manifested in anomalous scaling of the velocity structure functions of order p. Those functions were predicted to scale as the mean energy dissipation to the one-third p in a paper by (*) Kolmogorov, who also posited that this regime contains an "inertial range" of length scales lying above his namesake dissipation scale, at which viscous effects become significant.  Characterized by enstrophy production and vortex stretching, for 10 points, name this regime of fluid flow that occurs at high Reynolds number, the counterpart of laminar flow.
This behavior can be modeled by solving the Burgers equation with random forcing, but more commonly modeled with the standard k-epsilon model.  
{turbulence} [or {turbulent} flow]